Measurement of the running b-quark mass using $e^+e^- \to b\bar{b}g$ events
| dc.creator | Brandenburg, A. | |
| dc.creator | Burrows, P. N. | |
| dc.creator | Muller, D. | |
| dc.creator | Oishi, N. | |
| dc.creator | Uwer, P. | |
| dc.date | 1999-05-26 | |
| dc.date | 1999-09-20 | |
| dc.date.accessioned | 2026-07-07T10:33:52Z | |
| dc.date.available | 2026-07-07T10:33:52Z | |
| dc.description | We have studied the determination of the running b-quark mass, $m_b(M_Z)$, using $Z^0$ decays into 3 or more hadronic jets. We calculated the ratio of $\geq3$-jet fractions in $e^+e^-\to b\bar{b}$ vs. $e^+e^-\to q_l\bar{q_l}$ ($q_l$ = u or d or s) events at next-to-leading order in perturbative QCD using six different infra-red- and collinear-safe jet-finding algorithms. We compared with corresponding measurements from the SLD Collaboration and found a significant algorithm-dependence of the fitted $m_b(M_Z)$ value. Our best estimate, taking correlations into account, is $m_b(M_Z) = 2.56 \pm 0.27 (stat.) ^{+0.28}_{-0.38} (syst.) ^{+0.49}_{-1.48} (theor.) GeV/c^2$. | |
| dc.description | 22 pages (LaTeX), 1 Postscript figure. Version to appear in Phys. Lett. B. Several clarifying remarks added in the text, typos corrected, and theoretical results for very small masses added in the figure | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9905495 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9905495 | |
| dc.identifier | Phys.Lett.B468:168-177,1999 | |
| dc.identifier | doi:10.1016/S0370-2693(99)01194-6 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/179275 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | High Energy Physics - Experiment | |
| dc.title | Measurement of the running b-quark mass using $e^+e^- \to b\bar{b}g$ events | |
| dc.type | text |